\sect{Fermions in a gravitational field} %Baruch's B12. Consider fermions of mass $\mass$ and spin $1/2$ in a gravitational field with constant acceleration $g$ and at uniform temperature $T$. The density of the Fermions at zero height is $n(0)=n_{0}$. In item (3) assume that at zero height the fermions form a degenerate gas with Fermi energy $\epsilon_{F}^{0}$ that is much larger compared with~$T$. \begin{enumerate} \item Assume that the fermions behave as classical particles and find their density $n(h)$ as function of the height. \item Assume $T=0$. Find the local Fermi momentum $p_{F}(h)$ and the density $n(h)$ as function of the height. \item Assume low temperatures. Estimate the height $h_{c}$ such that for $h\gg h_{c}$ the fermions are non-degenerate. \item In the latter case find $n(h)$ for $h\gg h_{c}$, given as before $n_0$ at zero height. \end{enumerate} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%